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Zero-point renormalization of the band gap of semiconductors and insulators using the projector augmented wave method

MetadataDetails
Publication Date2022-09-29
JournalPhysical review. B./Physical review. B
AuthorsManuel Engel, Henrique Miranda, Laurent Chaput, Atsushi Togo, Carla Verdi
InstitutionsCentre National de la Recherche Scientifique, Université de Lorraine
Citations32
AnalysisFull AI Review Included

Technical Documentation & Analysis: Zero-point Renormalization in Diamond

Section titled “Technical Documentation & Analysis: Zero-point Renormalization in Diamond”

This document analyzes the research paper “Zero-point Renormalization of the Band Gap of Semiconductors and Insulators Using the PAW Method” (arXiv:2205.04265v2) to provide technical specifications and highlight how 6CCVD’s advanced MPCVD diamond materials directly support and extend this critical computational research into real-world applications.


This study provides crucial computational validation for predicting the fundamental electronic properties of wide-bandgap materials, specifically diamond (C-cd), using advanced first-principles methods.

  • Core Achievement: Successful calculation of the Zero-Point Renormalization (ZPR) of the band gap for 28 solids, including diamond, using the Projector-Augmented-Wave (PAW) method within Density Functional Theory (DFT).
  • Diamond ZPR Value: A converged non-adiabatic ZPR value of -323 meV was determined for cubic diamond (C-cd), essential for predicting the temperature dependence of diamond electronic devices.
  • Methodological Validation: The research validates the use of the Pseudized (PS) PAW formulation, demonstrating its significantly faster convergence with respect to intermediate conduction-band states compared to the All-Electron (AE) formulation.
  • Computational Rigor: Calculations employed large supercells (e.g., 4x4x4) and dense q-point grids (up to 64x64x64) to ensure accurate extrapolation and proper treatment of long-range electrostatic interactions (Fröhlich model).
  • Application Relevance: Accurate ZPR calculation is vital for designing high-performance electronic and optical devices, as it governs the intrinsic band gap magnitude at absolute zero and influences thermal stability.
  • 6CCVD Connection: The findings directly inform the material requirements for electronic-grade Single Crystal Diamond (SCD) and Polycrystalline Diamond (PCD) used in high-power and high-frequency applications.

The following hard data points were extracted, focusing primarily on the computational parameters and results for cubic diamond (C-cd).

ParameterValueUnitContext
Material StudiedDiamond (C-cd)N/ACubic Diamond Structure
Converged Band-Gap ZPR (PS)-323meVNon-adiabatic AHC Theory (Table VII)
Lattice Constant (a)3.57ÅOptimized DFT value (Table III)
Static Dielectric Constant (Δxx)5.70N/AIon-clamped (Table III)
Born Effective Charge (Z*xx)2.69N/ACalculated for C-cd (Table III)
PAW Potential Cutoff (Ecut)3000eVHighest Ecut used for C-cd (C_h_GW potential)
Supercell Size4x4x4N/AUsed for force constants/KS potential change
Maximum Extrapolation Grid64x64x64N/Aq-point/k-point mesh density
Smearing Parameter (ÎŽ)10meVUsed in the Fan-Migdal denominator

The computational approach relies on rigorous first-principles calculations using the PAW method, implemented primarily within the VASP code.

  1. Theoretical Framework: Non-adiabatic Allen-Heine-Cardona (AHC) theory was used to calculate the ZPR, incorporating both the Fan-Migdal (FM) and Debye-Waller (DW) contributions.
  2. PAW Formalism Comparison: Two distinct formulations for the electron-phonon matrix elements were compared: the All-Electron (AE) approach (derivatives taken before PAW transformation) and the Pseudized (PS) approach (derivatives taken after PAW transformation). The PS approach was selected for final converged results due to its superior convergence speed.
  3. Derivative Calculation: Finite atomic displacements in large supercells (e.g., 4x4x4) were used to numerically evaluate the required derivatives (inter-atomic force constants and changes in the self-consistent Kohn-Sham potential).
  4. Long-Range Interaction Treatment: For polar materials, the long-range electrostatic contributions to the electron-phonon matrix element were explicitly accounted for using a generalized Fröhlich model.
  5. Convergence and Extrapolation: ZPR values were converged with respect to the number of intermediate conduction-band states and extrapolated to infinite q-point density (up to 64x64x64 grids) based on a linear scaling assumption (ZPR vs. nq-1/3).

The accurate prediction of diamond’s intrinsic electronic properties, such as the ZPR, is foundational for developing next-generation diamond-based devices. 6CCVD provides the physical MPCVD diamond materials necessary to realize these high-performance applications.

Applicable Materials for Electronic and Optical Research

Section titled “Applicable Materials for Electronic and Optical Research”

The computational results for C-cd (diamond) require physical materials with exceptional purity and crystalline quality to match the theoretical ideal.

Research Requirement6CCVD Material SolutionKey Specifications
High-Purity Electronic SubstratesElectronic Grade Single Crystal Diamond (SCD)Ultra-low nitrogen content (critical for electronic band structure integrity). Available in thicknesses from 0.1 ”m to 500 ”m.
High-Power/Thermal ManagementThermal Grade Polycrystalline Diamond (PCD)Plates/wafers up to 125 mm diameter, ideal for large-area heat spreaders informed by precise thermal modeling.
Electrochemical/Doping StudiesBoron-Doped Diamond (BDD)Custom doping levels available for replicating semiconductor behavior and exploring BDD’s unique electrochemical properties.
Optical ApplicationsOptical Grade SCDHigh transmission across UV-Vis-IR spectra, suitable for windows or lenses where band gap stability is crucial.

The transition from theoretical modeling (like ZPR calculation) to functional devices often requires precise material engineering. 6CCVD offers full customization capabilities to meet specific research and development needs:

  • Custom Dimensions: We supply diamond plates and wafers in custom sizes, including large-area PCD up to 125 mm diameter, and SCD substrates up to 10 mm thick.
  • Surface Engineering: We provide ultra-smooth polishing services, achieving roughness values of Ra < 1 nm for SCD and Ra < 5 nm for inch-size PCD, essential for minimizing surface scattering and defect states.
  • Advanced Metalization: For creating ohmic contacts or complex device architectures, 6CCVD offers in-house metalization services, including deposition of Au, Pt, Pd, Ti, W, and Cu layers, tailored to specific interface requirements.

The complexity of electron-phonon interactions and band-gap renormalization requires deep material expertise. 6CCVD’s in-house PhD team specializes in MPCVD growth and material characterization, offering authoritative support:

  • Material Selection: Assistance in selecting the optimal diamond grade (SCD, PCD, or BDD) and crystal orientation for projects focused on high-frequency electronics, power devices, or quantum applications where band gap stability is paramount.
  • Process Optimization: Consultation on how material purity, defect density, and surface termination impact predicted electronic properties derived from first-principles calculations like those presented in this paper.
  • Global Logistics: Reliable global shipping (DDU default, DDP available) ensures that high-quality diamond materials reach research facilities worldwide efficiently.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.

View Original Abstract

We evaluate the zero-point renormalization (ZPR) due to electron-phonon\ninteractions of 28 solids using the projector-augmented-wave (PAW) method. The\ncalculations cover diamond, many zincblende semiconductors, rock-salt and\nwurtzite oxides, as well as silicate and titania. Particular care is taken to\ninclude long-range electrostatic interactions via a generalized Fr\“ohlich\nmodel, as discussed in Phys. Rev. Lett. 115, 176401 (2015) and Phys. Rev. B 92,\n054307 (2015). The data are compared to recent calculations, npj Computational\nMaterials 6, 167 (2020), and generally very good agreement is found. We discuss\nin detail the evaluation of the electron-phonon matrix elements within the PAW\nmethod. We show that two distinct versions can be obtained depending on when\nthe atomic derivatives are taken. If the PAW transformation is applied before\ntaking derivatives with respect to the ionic positions, equations similar to\nthe ones conventionally used in pseudopotential codes are obtained. If the PAW\ntransformation is used after taking the derivatives, the full-potential spirit\nis largely maintained. We show that both variants yield very similar ZPRs for\nselected materials when the rigid-ion approximation is employed. In practice,\nwe find however that the pseudo version converges more rapidly with respect to\nthe number of included unoccupied states.\n